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Brownian Motion on Treebolic Space:Positive Harmonic Functions Tome 66, No 4 (2016), P R AN IE N R A U L E O S F D T E U L T I ’ I T N S ANNALES DE L’INSTITUT FOURIER Alexander BENDIKOV, Laurent SALOFF-COSTE, Maura SALVATORI & Wolfgang WOESS Brownian motion on treebolic space:positive harmonic functions Tome 66, no 4 (2016), p. 1691-1731. <http://aif.cedram.org/item?id=AIF_2016__66_4_1691_0> © Association des Annales de l’institut Fourier, 2016, Certains droits réservés. Cet article est mis à disposition selon les termes de la licence CREATIVE COMMONS ATTRIBUTION – PAS DE MODIFICATION 3.0 FRANCE. http://creativecommons.org/licenses/by-nd/3.0/fr/ L’accès aux articles de la revue « Annales de l’institut Fourier » (http://aif.cedram.org/), implique l’accord avec les conditions générales d’utilisation (http://aif.cedram.org/legal/). cedram Article mis en ligne dans le cadre du Centre de diffusion des revues académiques de mathématiques http://www.cedram.org/ Ann. Inst. Fourier, Grenoble 66, 4 (2016) 1691-1731 BROWNIAN MOTION ON TREEBOLIC SPACE: POSITIVE HARMONIC FUNCTIONS by Alexander BENDIKOV, Laurent SALOFF-COSTE, Maura SALVATORI & Wolfgang WOESS (*) Abstract. — This paper studies potential theory on treebolic space, that is, the horocyclic product of a regular tree and hyperbolic upper half plane. Relying on the analysis on strip complexes developed by the authors, a family of Laplacians with “vertical drift” parameters is considered. We investigate the positive harmonic functions associated with those Laplacians. Résumé. — Ce travail est dedié à une étude de la théorie du potentiel sur l’espace arbolique, i.e., le produit horcyclique d’un ârbre régulier avec le demi- plan hyperbolique supérieur. En se basant sur l’analyse sur les complexes à bandes Riemanniennes développée par les auteurs, on considère une famille de Laplaciens avec deux paramètres concernant la dérive verticale. On examine les fonctions harmoniques associées à ces Laplaciens. 1. Introduction We recall the basic description of treebolic space. For many further de- tails on the geometry, metric structure and isometry group, the reader is referred to [3]. We consider the homogeneous tree T = Tp , drawn in such a way that each vertex v has one predecessor v− and p successors. We consider T as a metric graph, where each edge is a copy of the unit interval [0 , 1]. The discrete, integer-valued graph metric dT on the vertex set (0-skeleton) V (T) of T has an obvious “linear” extension to the entire metric graph. We can Keywords: Tree, hyperbolic plane, horocyclic product, quantum complex, Laplacian, positive harmonic functions. Math. classification: 31C05, 60J50,53C23, 05C05. (*) Partially supported by Austrian Science Fund (FWF) projects P24028 and W1230 and Polish NCN grant DEC-2012/05/B/ST 1/00613. 1692 A. Bendikov, L. Saloff-Coste, M. Salvatori & W. Woess ........ ....... ........ ........ ....... ... .......... ....... ... .......... ....... ... ....... .......... ... ....... ... ....... .. ....... ........ .. ....... ... ....... ... ....... ....... ... ....... ... ....... .......... ....... .......... ... ....... ........ ....... ........ ... ....... ....... ....... ....... ... ....... ....... ....... ....... ... ....... ....... ....... ....... ... ....... ....... ....... ....... ... ....... ....... ....... ....... ... ....... ....... ....... ....... ... ....... ....... ....... ....... ... ....... ....... ....... ....... ... ....... ....... ....... ....... ......... ....... ....... ....... ....... ....... .. ....... ....... ....... ....... ....... ... ....... ....... ....... ....... ....... ... ....... ....... ....... ....... ....... ... ....... ....... ....... ....... ....... ... ....... ....... ....... ....... ....... ... ....... ....... ....... ....... ....... ... ....... ....... ....... ....... ....... ... ....... ....... ....... ....... ....... ... .... ..... .... ... ....... ... ... ... ... ... ....... ... ... ... ... ... ....... ... ... ... ... ... ....... ... .. .. .. .. ....... ... ... ... ... ... ....... ... ... ... ... ... ....... ... ... ... ......... ... ....... ... ... ... ....... ... ... ....... ... ... ... ....... ... ... ....... ... ... ... ....... ... ... ....... ....... ... ... ....... ... ... ....... ....... ... ... ....... ... ... ....... ....... ... ... ....... ... ... ....... ....... ........... ........... ....... .... ..... ....... ... ... ....... ... ... ....... ... ... ....... ... ... ....... ... ... ....... ... ... ....... ... ... ....... ... ... ....... ... ... ....... ... ... ....... ... ... ....... ... ... ....... ... ... ....... ... ... ....... ... ... ....... ... ... ....... ... ... ....... ...... ....... ............ Figure 1. A compact piece of treebolic space, with p = 2.(1) partition the vertex set into countably many sets Hk , k ∈ Z, such that each Hk is countably infinite, and every vertex v ∈ Hk has its predecessor − − v in Hk−1 and its successors in Hk+1. We write [v , v] for the metric edge between those two vertices, parametrised by the unit interval. For − any w ∈ [v , v] we let t = k − dT(w, v) and set h(w) = t. In particular, h(v) = k for v ∈ Hk . In general, we set Ht = {w ∈ T : h(w) = t}. These sets are the horocycles. We choose a root vertex o ∈ H0 . Second, we consider hyperbolic upper half space H, and draw the hori- k zontal lines Lk = {x + i q : x ∈ R}, thereby subdividing H into the strips k−1 k Sk = {x + i y : x ∈ R , q 6 y 6 q }, where k ∈ Z. We sometimes write H(q) for the resulting strip complex, which is of course hyperbolic plane in every geometric aspect. The reader is invited to have a look at the respective figures of Tp and “sliced” hyperbolic plane H(q) in [3]. Treebolic space with parameters q and p is then (1.1) HT(q, p) = {z = (z, w) ∈ H × Tp : h(w) = logq(Im z)} . Thus, in treebolic space HT(q, p), infinitely many copies of the strips Sk are glued together as follows: to each vertex v of T there corresponds the bifurcation line k Lv = {(x + i q , v): x ∈ R} = Lk × {v} , where h(v) = k . (1) This figure also appears in [2]. ANNALES DE L’INSTITUT FOURIER HARMONIC FUNCTIONS ON TREEBOLIC SPACE 1693 Along this line, the strips k−1 k − Sv = (x + i y, w): x ∈ R , y ∈ [q , q ] , w ∈ [v , v] , h(w) = logq y − and Su , where u ∈ V (T) with u = v, are glued together. The origin of our space is o = (0, o). In [3], we outlined several viewpoints why this space is interesting. It can be considered as a concrete example of a Riemannian complex in the spirit of Eells and Fuglede [15]. Treebolic space is a strip complex (“quantum com- plex”) in the sense of [2], where a careful study of Laplace operators on such spaces is undertaken, taking into account the serious subtleties arising from the singularites of such a complex along its bifurcation manifolds. In our case, the latter are the lines Lv , v ∈ V (T). The other interesting feature is that treebolic spaces are horocyclic products of H(q) and Tp , with a struc- ture that shares many features with the Diestel-Leader graphs DL(p, q) [13] as well as with the manifold (Lie group) Sol(p, q), the horocyclic product of two hyperbolic planes with curvatures −p2 and −q2, respectively, where p, q > 0. Compare with Woess [25], Brofferio and Woess [7], [8] and with Brofferio, Salvatori and Woess [6]; see also the survey by Woess [26]. The graph DL(p, p) is a Cayley graph of the Lamplighter group Zp oZ. Similarly, the Baumslag-Solitar group BS(p) = ha, b | ab = bpai is a prominent group that acts isometrically and with compact quotient on HT(p, p). In the present paper, we take up the thread from [3], where we have investigated the details of the metric structure, geometry and isometries before describing the spatial asymptotic behaviour of Brownian motion on treebolic space. Brownian motion is induced by a Laplace operator ∆α,β , where the parameter α is the coefficient of a vertical drift term in the inte- rior of each strip, while β is responsible for (again vertical) Kirchhoff type bifurcation conditions along the lines Lv . The serious task of rigorously constructing ∆α,β as an essentially self-adjoint diffusion operator was un- dertaken in the general setting of strip complexes in [2]. For the specific case of HT, it is explained in detail in [3]. We shall recall only its basic features, while we shall use freely the geometric details from [3]. Here, we face the rather difficult issue to describe, resp. determine the positive harmonic functions on HT(q, p). In §2, we recall the basic features of treebolic space and the family of Laplacians with Kirchhoff conditions at the bifurcation lines. In §3, we start with a Poisson representation on “rectangular” sets which are compact. Then we obtain such a representa- tion on simply connected sets which are unions of strips and a solution of the Dirichlet problem on those sets. (For the technical details of the main TOME 66 (2016), FASCICULE 4 1694 A. Bendikov, L. Saloff-Coste, M. Salvatori & W. Woess results presented here, the reader is referred to the respective sections.) For the following, let Ω be the union of all closed strips adjactent to Lo and Ω Ω its interior, and let µw be the exit distribution from Ω of Brownian motion starting at w ∈ Ω. Theorems 3.9& 3.11. (I) Let h be continuous on Ω and harmonic on Ω, and suppose that on that set, h grows at most exponentially with respect to the metric of HT. Then for every w ∈ Ω, Z Ω h(w) = h(z) dµw(z) . ∂Ω (II) Let f be continuous on ∂Ω, and suppose that on that set, f grows at most exponentially with respect to the metric of HT. Then Z Ω h(w) = f(z) dµw(z) , w ∈ Ω ∂Ω defines an extension of f that is harmonic on Ω and continuous on Ω. The difficulties arise from
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